解码ρ介子态在解释e+e−→a2(1320)π数据和其他反应中的作用

IF 5.3 2区 物理与天体物理 Q1 Physics and Astronomy
Qin-Song Zhou, Zi-Yue Bai, Jun-Zhang Wang, Hao Xu, Xiang Liu
{"title":"解码ρ介子态在解释e+e−→a2(1320)π数据和其他反应中的作用","authors":"Qin-Song Zhou, Zi-Yue Bai, Jun-Zhang Wang, Hao Xu, Xiang Liu","doi":"10.1103/pdfh-mk79","DOIUrl":null,"url":null,"abstract":"Recently, the BESIII Collaboration observed a ρ</a:mi></a:math>-like structure <c:math xmlns:c=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><c:mi>Y</c:mi><c:mo stretchy=\"false\">(</c:mo><c:mn>2044</c:mn><c:mo stretchy=\"false\">)</c:mo></c:math> in <g:math xmlns:g=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><g:msup><g:mi>e</g:mi><g:mo>+</g:mo></g:msup><g:msup><g:mi>e</g:mi><g:mo>−</g:mo></g:msup><g:mo stretchy=\"false\">→</g:mo><g:msub><g:mi>a</g:mi><g:mn>2</g:mn></g:msub><g:mo stretchy=\"false\">(</g:mo><g:mn>1320</g:mn><g:mo stretchy=\"false\">)</g:mo><g:mi>π</g:mi></g:math>, suggesting that <l:math xmlns:l=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><l:mi>Y</l:mi><l:mo stretchy=\"false\">(</l:mo><l:mn>2044</l:mn><l:mo stretchy=\"false\">)</l:mo></l:math> may be a candidate of vector meson <p:math xmlns:p=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><p:mi>ρ</p:mi><p:mo stretchy=\"false\">(</p:mo><p:mn>2</p:mn><p:mi>D</p:mi><p:mo stretchy=\"false\">)</p:mo></p:math> by comparing resonance parameters. However, the theoretical prediction for the combined branching ratio <t:math xmlns:t=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><t:msub><t:mi mathvariant=\"normal\">Γ</t:mi><t:mrow><t:msup><t:mi>e</t:mi><t:mo>+</t:mo></t:msup><t:msup><t:mi>e</t:mi><t:mo>−</t:mo></t:msup></t:mrow></t:msub><t:msub><t:mi mathvariant=\"script\">B</t:mi><t:mrow><t:msub><t:mi>a</t:mi><t:mn>2</t:mn></t:msub><t:mo stretchy=\"false\">(</t:mo><t:mn>1320</t:mn><t:mo stretchy=\"false\">)</t:mo><t:mi>π</t:mi></t:mrow></t:msub></t:math> for the pure <z:math xmlns:z=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><z:mi>ρ</z:mi><z:mo stretchy=\"false\">(</z:mo><z:mn>2</z:mn><z:mi>D</z:mi><z:mo stretchy=\"false\">)</z:mo></z:math> state is about 2 orders of magnitude smaller than the experimental value. To resolve this discrepancy and decipher the nature of <db:math xmlns:db=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><db:mi>Y</db:mi><db:mo stretchy=\"false\">(</db:mo><db:mn>2044</db:mn><db:mo stretchy=\"false\">)</db:mo></db:math>, this work proposes an <hb:math xmlns:hb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><hb:mrow><hb:mi>S</hb:mi><hb:mtext>−</hb:mtext><hb:mi>D</hb:mi></hb:mrow></hb:math> mixing scheme to reanalyze the cross section of <jb:math xmlns:jb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><jb:msup><jb:mi>e</jb:mi><jb:mo>+</jb:mo></jb:msup><jb:msup><jb:mi>e</jb:mi><jb:mo>−</jb:mo></jb:msup><jb:mo stretchy=\"false\">→</jb:mo><jb:msub><jb:mi>a</jb:mi><jb:mn>2</jb:mn></jb:msub><jb:mo stretchy=\"false\">(</jb:mo><jb:mn>1320</jb:mn><jb:mo stretchy=\"false\">)</jb:mo><jb:mi>π</jb:mi></jb:math>, and finds that the aforementioned branching ratio discrepancy can be resolved. Our results show that the <ob:math xmlns:ob=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><ob:mi>Y</ob:mi><ob:mo stretchy=\"false\">(</ob:mo><ob:mn>2044</ob:mn><ob:mo stretchy=\"false\">)</ob:mo></ob:math> structure can be reproduced by introducing four theoretically predicted <sb:math xmlns:sb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><sb:mrow><sb:mi>S</sb:mi><sb:mtext>−</sb:mtext><sb:mi>D</sb:mi></sb:mrow></sb:math> mixing <ub:math xmlns:ub=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><ub:mi>ρ</ub:mi></ub:math> meson states <wb:math xmlns:wb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><wb:msubsup><wb:mi>ρ</wb:mi><wb:mrow><wb:mn>3</wb:mn><wb:mi>S</wb:mi><wb:mo>−</wb:mo><wb:mn>2</wb:mn><wb:mi>D</wb:mi></wb:mrow><wb:mo>′</wb:mo></wb:msubsup></wb:math>, <yb:math xmlns:yb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><yb:msubsup><yb:mi>ρ</yb:mi><yb:mrow><yb:mn>3</yb:mn><yb:mi>S</yb:mi><yb:mo>−</yb:mo><yb:mn>2</yb:mn><yb:mi>D</yb:mi></yb:mrow><yb:mrow><yb:mo>′′</yb:mo></yb:mrow></yb:msubsup></yb:math>, ρ</ac:mi>4</ac:mn>S</ac:mi>−</ac:mo>3</ac:mn>D</ac:mi></ac:mrow>′</ac:mo></ac:msubsup></ac:math>, and <cc:math xmlns:cc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><cc:msubsup><cc:mi>ρ</cc:mi><cc:mrow><cc:mn>4</cc:mn><cc:mi>S</cc:mi><cc:mo>−</cc:mo><cc:mn>3</cc:mn><cc:mi>D</cc:mi></cc:mrow><cc:mrow><cc:mo>′′</cc:mo></cc:mrow></cc:msubsup></cc:math> as intermediate resonances, in which dominant contribution arises from <ec:math xmlns:ec=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><ec:msubsup><ec:mi>ρ</ec:mi><ec:mrow><ec:mn>3</ec:mn><ec:mi>S</ec:mi><ec:mo>−</ec:mo><ec:mn>2</ec:mn><ec:mi>D</ec:mi></ec:mrow><ec:mrow><ec:mo>′′</ec:mo></ec:mrow></ec:msubsup></ec:math> and their inference effect is also significant. Furthermore, we reanalyzed five additional isospin vector processes <gc:math xmlns:gc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><gc:msup><gc:mi>e</gc:mi><gc:mo>+</gc:mo></gc:msup><gc:msup><gc:mi>e</gc:mi><gc:mo>−</gc:mo></gc:msup><gc:mo stretchy=\"false\">→</gc:mo><gc:mi>ω</gc:mi><gc:msup><gc:mi>π</gc:mi><gc:mn>0</gc:mn></gc:msup></gc:math>, <jc:math xmlns:jc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><jc:msup><jc:mi>e</jc:mi><jc:mo>+</jc:mo></jc:msup><jc:msup><jc:mi>e</jc:mi><jc:mo>−</jc:mo></jc:msup><jc:mo stretchy=\"false\">→</jc:mo><jc:msub><jc:mi>f</jc:mi><jc:mn>1</jc:mn></jc:msub><jc:mo stretchy=\"false\">(</jc:mo><jc:mn>1285</jc:mn><jc:mo stretchy=\"false\">)</jc:mo><jc:msup><jc:mi>π</jc:mi><jc:mo>+</jc:mo></jc:msup><jc:msup><jc:mi>π</jc:mi><jc:mo>−</jc:mo></jc:msup></jc:math>, <oc:math xmlns:oc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><oc:msup><oc:mi>e</oc:mi><oc:mo>+</oc:mo></oc:msup><oc:msup><oc:mi>e</oc:mi><oc:mo>−</oc:mo></oc:msup><oc:mo stretchy=\"false\">→</oc:mo><oc:msup><oc:mi>π</oc:mi><oc:mo>+</oc:mo></oc:msup><oc:msup><oc:mi>π</oc:mi><oc:mo>−</oc:mo></oc:msup></oc:math>, <rc:math xmlns:rc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><rc:msup><rc:mi>e</rc:mi><rc:mo>+</rc:mo></rc:msup><rc:msup><rc:mi>e</rc:mi><rc:mo>−</rc:mo></rc:msup><rc:mo stretchy=\"false\">→</rc:mo><rc:mi>ρ</rc:mi><rc:mi>η</rc:mi></rc:math>, and <uc:math xmlns:uc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><uc:msup><uc:mi>e</uc:mi><uc:mo>+</uc:mo></uc:msup><uc:msup><uc:mi>e</uc:mi><uc:mo>−</uc:mo></uc:msup><uc:mo stretchy=\"false\">→</uc:mo><uc:msup><uc:mi>η</uc:mi><uc:mo>′</uc:mo></uc:msup><uc:msup><uc:mi>π</uc:mi><uc:mo>+</uc:mo></uc:msup><uc:msup><uc:mi>π</uc:mi><uc:mo>−</uc:mo></uc:msup></uc:math> based on the same <xc:math xmlns:xc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><xc:mrow><xc:mi>S</xc:mi><xc:mtext>−</xc:mtext><xc:mi>D</xc:mi></xc:mrow></xc:math> mixing framework, and simultaneously reproduced their experimental cross section data. This work provides a unified framework to elucidate all observed <zc:math xmlns:zc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><zc:mi>ρ</zc:mi></zc:math>-like structures near 2 GeV in the <bd:math xmlns:bd=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><bd:msup><bd:mi>e</bd:mi><bd:mo>+</bd:mo></bd:msup><bd:msup><bd:mi>e</bd:mi><bd:mo>−</bd:mo></bd:msup></bd:math> annihilation processes, and suggests that the <dd:math xmlns:dd=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><dd:mrow><dd:mi>S</dd:mi><dd:mtext>−</dd:mtext><dd:mi>D</dd:mi></dd:mrow></dd:math> mixing effect may be crucial for understanding the mass spectrum and decay behaviors of the higher <fd:math xmlns:fd=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><fd:mi>ρ</fd:mi></fd:math> meson states.","PeriodicalId":20167,"journal":{"name":"Physical Review D","volume":"35 1","pages":""},"PeriodicalIF":5.3000,"publicationDate":"2025-10-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Decoding the role of ρ mesonic states for elucidating the e+e−→a2(1320)π data and other reactions\",\"authors\":\"Qin-Song Zhou, Zi-Yue Bai, Jun-Zhang Wang, Hao Xu, Xiang Liu\",\"doi\":\"10.1103/pdfh-mk79\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Recently, the BESIII Collaboration observed a ρ</a:mi></a:math>-like structure <c:math xmlns:c=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><c:mi>Y</c:mi><c:mo stretchy=\\\"false\\\">(</c:mo><c:mn>2044</c:mn><c:mo stretchy=\\\"false\\\">)</c:mo></c:math> in <g:math xmlns:g=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><g:msup><g:mi>e</g:mi><g:mo>+</g:mo></g:msup><g:msup><g:mi>e</g:mi><g:mo>−</g:mo></g:msup><g:mo stretchy=\\\"false\\\">→</g:mo><g:msub><g:mi>a</g:mi><g:mn>2</g:mn></g:msub><g:mo stretchy=\\\"false\\\">(</g:mo><g:mn>1320</g:mn><g:mo stretchy=\\\"false\\\">)</g:mo><g:mi>π</g:mi></g:math>, suggesting that <l:math xmlns:l=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><l:mi>Y</l:mi><l:mo stretchy=\\\"false\\\">(</l:mo><l:mn>2044</l:mn><l:mo stretchy=\\\"false\\\">)</l:mo></l:math> may be a candidate of vector meson <p:math xmlns:p=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><p:mi>ρ</p:mi><p:mo stretchy=\\\"false\\\">(</p:mo><p:mn>2</p:mn><p:mi>D</p:mi><p:mo stretchy=\\\"false\\\">)</p:mo></p:math> by comparing resonance parameters. However, the theoretical prediction for the combined branching ratio <t:math xmlns:t=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><t:msub><t:mi mathvariant=\\\"normal\\\">Γ</t:mi><t:mrow><t:msup><t:mi>e</t:mi><t:mo>+</t:mo></t:msup><t:msup><t:mi>e</t:mi><t:mo>−</t:mo></t:msup></t:mrow></t:msub><t:msub><t:mi mathvariant=\\\"script\\\">B</t:mi><t:mrow><t:msub><t:mi>a</t:mi><t:mn>2</t:mn></t:msub><t:mo stretchy=\\\"false\\\">(</t:mo><t:mn>1320</t:mn><t:mo stretchy=\\\"false\\\">)</t:mo><t:mi>π</t:mi></t:mrow></t:msub></t:math> for the pure <z:math xmlns:z=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><z:mi>ρ</z:mi><z:mo stretchy=\\\"false\\\">(</z:mo><z:mn>2</z:mn><z:mi>D</z:mi><z:mo stretchy=\\\"false\\\">)</z:mo></z:math> state is about 2 orders of magnitude smaller than the experimental value. To resolve this discrepancy and decipher the nature of <db:math xmlns:db=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><db:mi>Y</db:mi><db:mo stretchy=\\\"false\\\">(</db:mo><db:mn>2044</db:mn><db:mo stretchy=\\\"false\\\">)</db:mo></db:math>, this work proposes an <hb:math xmlns:hb=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><hb:mrow><hb:mi>S</hb:mi><hb:mtext>−</hb:mtext><hb:mi>D</hb:mi></hb:mrow></hb:math> mixing scheme to reanalyze the cross section of <jb:math xmlns:jb=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><jb:msup><jb:mi>e</jb:mi><jb:mo>+</jb:mo></jb:msup><jb:msup><jb:mi>e</jb:mi><jb:mo>−</jb:mo></jb:msup><jb:mo stretchy=\\\"false\\\">→</jb:mo><jb:msub><jb:mi>a</jb:mi><jb:mn>2</jb:mn></jb:msub><jb:mo stretchy=\\\"false\\\">(</jb:mo><jb:mn>1320</jb:mn><jb:mo stretchy=\\\"false\\\">)</jb:mo><jb:mi>π</jb:mi></jb:math>, and finds that the aforementioned branching ratio discrepancy can be resolved. Our results show that the <ob:math xmlns:ob=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><ob:mi>Y</ob:mi><ob:mo stretchy=\\\"false\\\">(</ob:mo><ob:mn>2044</ob:mn><ob:mo stretchy=\\\"false\\\">)</ob:mo></ob:math> structure can be reproduced by introducing four theoretically predicted <sb:math xmlns:sb=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><sb:mrow><sb:mi>S</sb:mi><sb:mtext>−</sb:mtext><sb:mi>D</sb:mi></sb:mrow></sb:math> mixing <ub:math xmlns:ub=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><ub:mi>ρ</ub:mi></ub:math> meson states <wb:math xmlns:wb=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><wb:msubsup><wb:mi>ρ</wb:mi><wb:mrow><wb:mn>3</wb:mn><wb:mi>S</wb:mi><wb:mo>−</wb:mo><wb:mn>2</wb:mn><wb:mi>D</wb:mi></wb:mrow><wb:mo>′</wb:mo></wb:msubsup></wb:math>, <yb:math xmlns:yb=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><yb:msubsup><yb:mi>ρ</yb:mi><yb:mrow><yb:mn>3</yb:mn><yb:mi>S</yb:mi><yb:mo>−</yb:mo><yb:mn>2</yb:mn><yb:mi>D</yb:mi></yb:mrow><yb:mrow><yb:mo>′′</yb:mo></yb:mrow></yb:msubsup></yb:math>, ρ</ac:mi>4</ac:mn>S</ac:mi>−</ac:mo>3</ac:mn>D</ac:mi></ac:mrow>′</ac:mo></ac:msubsup></ac:math>, and <cc:math xmlns:cc=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><cc:msubsup><cc:mi>ρ</cc:mi><cc:mrow><cc:mn>4</cc:mn><cc:mi>S</cc:mi><cc:mo>−</cc:mo><cc:mn>3</cc:mn><cc:mi>D</cc:mi></cc:mrow><cc:mrow><cc:mo>′′</cc:mo></cc:mrow></cc:msubsup></cc:math> as intermediate resonances, in which dominant contribution arises from <ec:math xmlns:ec=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><ec:msubsup><ec:mi>ρ</ec:mi><ec:mrow><ec:mn>3</ec:mn><ec:mi>S</ec:mi><ec:mo>−</ec:mo><ec:mn>2</ec:mn><ec:mi>D</ec:mi></ec:mrow><ec:mrow><ec:mo>′′</ec:mo></ec:mrow></ec:msubsup></ec:math> and their inference effect is also significant. Furthermore, we reanalyzed five additional isospin vector processes <gc:math xmlns:gc=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><gc:msup><gc:mi>e</gc:mi><gc:mo>+</gc:mo></gc:msup><gc:msup><gc:mi>e</gc:mi><gc:mo>−</gc:mo></gc:msup><gc:mo stretchy=\\\"false\\\">→</gc:mo><gc:mi>ω</gc:mi><gc:msup><gc:mi>π</gc:mi><gc:mn>0</gc:mn></gc:msup></gc:math>, <jc:math xmlns:jc=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><jc:msup><jc:mi>e</jc:mi><jc:mo>+</jc:mo></jc:msup><jc:msup><jc:mi>e</jc:mi><jc:mo>−</jc:mo></jc:msup><jc:mo stretchy=\\\"false\\\">→</jc:mo><jc:msub><jc:mi>f</jc:mi><jc:mn>1</jc:mn></jc:msub><jc:mo stretchy=\\\"false\\\">(</jc:mo><jc:mn>1285</jc:mn><jc:mo stretchy=\\\"false\\\">)</jc:mo><jc:msup><jc:mi>π</jc:mi><jc:mo>+</jc:mo></jc:msup><jc:msup><jc:mi>π</jc:mi><jc:mo>−</jc:mo></jc:msup></jc:math>, <oc:math xmlns:oc=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><oc:msup><oc:mi>e</oc:mi><oc:mo>+</oc:mo></oc:msup><oc:msup><oc:mi>e</oc:mi><oc:mo>−</oc:mo></oc:msup><oc:mo stretchy=\\\"false\\\">→</oc:mo><oc:msup><oc:mi>π</oc:mi><oc:mo>+</oc:mo></oc:msup><oc:msup><oc:mi>π</oc:mi><oc:mo>−</oc:mo></oc:msup></oc:math>, <rc:math xmlns:rc=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><rc:msup><rc:mi>e</rc:mi><rc:mo>+</rc:mo></rc:msup><rc:msup><rc:mi>e</rc:mi><rc:mo>−</rc:mo></rc:msup><rc:mo stretchy=\\\"false\\\">→</rc:mo><rc:mi>ρ</rc:mi><rc:mi>η</rc:mi></rc:math>, and <uc:math xmlns:uc=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><uc:msup><uc:mi>e</uc:mi><uc:mo>+</uc:mo></uc:msup><uc:msup><uc:mi>e</uc:mi><uc:mo>−</uc:mo></uc:msup><uc:mo stretchy=\\\"false\\\">→</uc:mo><uc:msup><uc:mi>η</uc:mi><uc:mo>′</uc:mo></uc:msup><uc:msup><uc:mi>π</uc:mi><uc:mo>+</uc:mo></uc:msup><uc:msup><uc:mi>π</uc:mi><uc:mo>−</uc:mo></uc:msup></uc:math> based on the same <xc:math xmlns:xc=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><xc:mrow><xc:mi>S</xc:mi><xc:mtext>−</xc:mtext><xc:mi>D</xc:mi></xc:mrow></xc:math> mixing framework, and simultaneously reproduced their experimental cross section data. This work provides a unified framework to elucidate all observed <zc:math xmlns:zc=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><zc:mi>ρ</zc:mi></zc:math>-like structures near 2 GeV in the <bd:math xmlns:bd=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><bd:msup><bd:mi>e</bd:mi><bd:mo>+</bd:mo></bd:msup><bd:msup><bd:mi>e</bd:mi><bd:mo>−</bd:mo></bd:msup></bd:math> annihilation processes, and suggests that the <dd:math xmlns:dd=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><dd:mrow><dd:mi>S</dd:mi><dd:mtext>−</dd:mtext><dd:mi>D</dd:mi></dd:mrow></dd:math> mixing effect may be crucial for understanding the mass spectrum and decay behaviors of the higher <fd:math xmlns:fd=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><fd:mi>ρ</fd:mi></fd:math> meson states.\",\"PeriodicalId\":20167,\"journal\":{\"name\":\"Physical Review D\",\"volume\":\"35 1\",\"pages\":\"\"},\"PeriodicalIF\":5.3000,\"publicationDate\":\"2025-10-17\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Physical Review D\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://doi.org/10.1103/pdfh-mk79\",\"RegionNum\":2,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q1\",\"JCRName\":\"Physics and Astronomy\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Physical Review D","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.1103/pdfh-mk79","RegionNum":2,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"Physics and Astronomy","Score":null,"Total":0}
引用次数: 0

摘要

最近,BESIII Collaboration在e+e−→a2(1320)π中观测到一个ρ类结构Y(2044),通过比较共振参数,表明Y(2044)可能是矢量介子ρ(2D)的候选粒子。然而,纯ρ(2D)态的组合分支比Γe+e−Ba2(1320)π的理论预测值比实验值小约2个数量级。为了解决这一差异并破译Y(2044)的性质,本文提出了一种S - D混合方案来重新分析e+e−→a2(1320)π的截面,并发现上述分支比差异可以解决。结果表明,引入理论预测的4个S - D混合ρ介子态ρ 3s - 2D’、ρ 3s - 2D’、ρ 4s - 3D’和ρ 4s - 3D’作为中间共振可以再现Y(2044)结构,其中ρ 3s - 2D’的贡献占主导地位,它们的推理效果也很显著。此外,在相同的S - D混合框架下,我们重新分析了另外5个同位旋矢量过程e+e−→ωπ0、e+e−→f1(1285)π+π−、e+e−→π+π−、e+e−→ρη和e+e−→η′π+π−,并同时重现了它们的实验截面数据。这项工作提供了一个统一的框架来解释在e+e−湮灭过程中所有观测到的2 GeV附近的ρ-类结构,并表明S - D混合效应可能对理解高ρ介子态的质谱和衰变行为至关重要。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Decoding the role of ρ mesonic states for elucidating the e+e−→a2(1320)π data and other reactions
Recently, the BESIII Collaboration observed a ρ-like structure Y(2044) in e+ea2(1320)π, suggesting that Y(2044) may be a candidate of vector meson ρ(2D) by comparing resonance parameters. However, the theoretical prediction for the combined branching ratio Γe+eBa2(1320)π for the pure ρ(2D) state is about 2 orders of magnitude smaller than the experimental value. To resolve this discrepancy and decipher the nature of Y(2044), this work proposes an SD mixing scheme to reanalyze the cross section of e+ea2(1320)π, and finds that the aforementioned branching ratio discrepancy can be resolved. Our results show that the Y(2044) structure can be reproduced by introducing four theoretically predicted SD mixing ρ meson states ρ3S2D, ρ3S2D′′, ρ4S−3D′, and ρ4S3D′′ as intermediate resonances, in which dominant contribution arises from ρ3S2D′′ and their inference effect is also significant. Furthermore, we reanalyzed five additional isospin vector processes e+eωπ0, e+ef1(1285)π+π, e+eπ+π, e+eρη, and e+eηπ+π based on the same SD mixing framework, and simultaneously reproduced their experimental cross section data. This work provides a unified framework to elucidate all observed ρ-like structures near 2 GeV in the e+e annihilation processes, and suggests that the SD mixing effect may be crucial for understanding the mass spectrum and decay behaviors of the higher ρ meson states.
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来源期刊
Physical Review D
Physical Review D 物理-天文与天体物理
CiteScore
9.20
自引率
36.00%
发文量
0
审稿时长
2 months
期刊介绍: Physical Review D (PRD) is a leading journal in elementary particle physics, field theory, gravitation, and cosmology and is one of the top-cited journals in high-energy physics. PRD covers experimental and theoretical results in all aspects of particle physics, field theory, gravitation and cosmology, including: Particle physics experiments, Electroweak interactions, Strong interactions, Lattice field theories, lattice QCD, Beyond the standard model physics, Phenomenological aspects of field theory, general methods, Gravity, cosmology, cosmic rays, Astrophysics and astroparticle physics, General relativity, Formal aspects of field theory, field theory in curved space, String theory, quantum gravity, gauge/gravity duality.
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